First published online December 3, 2004
Journal of Experimental Biology 207, 4515-4524 (2004)
Published by The Company of Biologists 2004
doi: 10.1242/jeb.01289
Kinetics and rhythm of body contractions in the sponge Tethya wilhelma (Porifera: Demospongiae)
Michael Nickel
Department of Zoology, Biological Institute, Stuttgart University,
D-70550 Stuttgart, Germany

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Fig. 1. (A) Contraction patterns of two specimens (Tw1 and Tw2) of T.
wilhelma, representing the changes in projected areas over an
experimental period of 18 h. Tw1 was placed in the aquarium, Tw2 in a closed
experimental reactor. Note the subcontraction (asterisk) of Tw2 at a time
point when a regular contraction should have taken place if the rhythm of the
former contraction series had continued; dotted lines, Tw1; broken lines, Tw2.
(B) Comparison of average contraction cycle duration of Tw1 (83.3±11
min; N=12) and Tw2 (169.0±28 min; N=6).
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Fig. 2. Long-term recording over more than 7 days of the changes in projected area
during contraction cycles of two specimens of T. wilhelma in the
aquarium (A) and the open glass chamber (B). Light and dark periods are
represented by white and grey backgrounds, respectively. Subcontractions,
which differ significantly from regular contractions, are marked by asterisks.
Experimental periods S1, S2 and S3 are represented by movies in the
supplementary material. S1 represents a regular contraction series, S2 shows a
series of subcontractions between regular contractions, S3 demonstrates the
reaction of the sponge on a mechanical stimulation (amphipod attack). Note the
adaptation phase in B after settling the sponge in the observation
chamber.
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Fig. 3. Comparison of average contraction cycle durations during day and night for
two specimens of T. wilhelma (Tw 1 and Tw 2) and for the combined
datasets (Tw 1+2). Contraction cycle duration differs significantly between
day and night (P=0.042).
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Fig. 6. (A) Local fields used to measure the spreading of local contractile waves
over the sponge body. Field a represents an measurement area of 3
mm2, field b represents 2 mm2; both are not completely
filled by sponge, to record changes due to contraction; distance d
between a and b is 3 mm; bar, 2.5 mm. (B) Changes in the projected areas of
fields a and b during a contraction event. The maximum contraction spreads as
a wave over the sponge surface, taking 4 min to traverse the 3 mm distance, a
speed of 750 µm min-1 (=12.5 µm s-1). The
contraction used for this measurement is shown in movie S4 in supplementary
material.
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Fig. 7. Contraction pattern and main contraction states of two fused individuals
(Tw 1 and Tw 2) of T. wilhelma. (A) Both individuals in expanded
phase. (B) Tw 1 in contracted phase, Tw 2 in expanded phase. (C) Both
individuals in contracted phase. (C) Tw 1 in expanded phase, Tw 2 in
contracted phase. Bars, 5 mm. (E) Contraction patterns of Tw 1 and Tw 2 and
both together (Tw 1+2) over 24 h. A*-D* are contraction
states represented by images A-D. The time-lapse series used for this
measurement is shown in movie S5 in supplementary material.
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© The Company of Biologists Ltd 2004